Axion optical induction of antiferromagnetic order.
Jian-Xiang QiuChristian TzschaschelJunyeong AhnAnyuan GaoHouchen LiXin-Yue ZhangBarun GhoshChaowei HuYu-Xuan WangYu-Fei LiuDamien BérubéThao DinhZhenhao GongShang-Wei LienSheng-Chin HoBahadur SinghKenji WatanabeTakashi TaniguchiDavid C BellHai-Zhou LuArun BansilHsin LinTay-Rong ChangBrian B ZhouQiong MaAshvin VishwanathNi NiSu-Yang XuPublished in: Nature materials (2023)
Using circularly polarized light to control quantum matter is a highly intriguing topic in physics, chemistry and biology. Previous studies have demonstrated helicity-dependent optical control of chirality and magnetization, with important implications in asymmetric synthesis in chemistry; homochirality in biomolecules; and ferromagnetic spintronics. We report the surprising observation of helicity-dependent optical control of fully compensated antiferromagnetic order in two-dimensional even-layered MnBi 2 Te 4 , a topological axion insulator with neither chirality nor magnetization. To understand this control, we study an antiferromagnetic circular dichroism, which appears only in reflection but is absent in transmission. We show that the optical control and circular dichroism both arise from the optical axion electrodynamics. Our axion induction provides the possibility to optically control a family of [Formula: see text]-symmetric antiferromagnets ([Formula: see text], inversion; [Formula: see text], time-reversal) such as Cr 2 O 3 , even-layered CrI 3 and possibly the pseudo-gap state in cuprates. In MnBi 2 Te 4 , this further opens the door for optical writing of a dissipationless circuit formed by topological edge states.